JPS5868703A - Optical switch - Google Patents
Optical switchInfo
- Publication number
- JPS5868703A JPS5868703A JP16833981A JP16833981A JPS5868703A JP S5868703 A JPS5868703 A JP S5868703A JP 16833981 A JP16833981 A JP 16833981A JP 16833981 A JP16833981 A JP 16833981A JP S5868703 A JPS5868703 A JP S5868703A
- Authority
- JP
- Japan
- Prior art keywords
- optical
- basic
- gratings
- optical fibers
- switch matrix
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04Q—SELECTING
- H04Q3/00—Selecting arrangements
- H04Q3/42—Circuit arrangements for indirect selecting controlled by common circuits, e.g. register controller, marker
- H04Q3/52—Circuit arrangements for indirect selecting controlled by common circuits, e.g. register controller, marker using static devices in switching stages, e.g. electronic switching arrangements
- H04Q3/526—Optical switching systems
Landscapes
- Engineering & Computer Science (AREA)
- Computer Networks & Wireless Communication (AREA)
- Mechanical Light Control Or Optical Switches (AREA)
- Electronic Switches (AREA)
- Use Of Switch Circuits For Exchanges And Methods Of Control Of Multiplex Exchanges (AREA)
Abstract
Description
【発明の詳細な説明】
不発明は光スイツチ装置、特に人、出線数音容易に大に
し得る光スイッチマトリクスに関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical switch device, and more particularly to an optical switch matrix that can easily increase the number of outgoing lines.
’4f話交換機などでは多数の入線のうちの任意の1つ
を多数の出線のうちの任意の1つに接続し、そして該任
意の1組の人、出線が接続されている間に他の人、出、
簾も同様に選択接続できることか必要である。このよう
な交換機能は、機械式のものならクロスバ−スイッチな
ど、デジタル式のものならメモリ利用のハイウェイスイ
ッチなどを用いて容易に実現できる。例えばクロスバ−
スイッチ利用の機械式捷たは電子式交換機では基本格子
と呼ぶ小規模スイッチマトリクスから容易に大規模スイ
ッチマトリクス全構成できる。第1図は2×2の基本格
子10(添字a、b・・・・・・・・・は相互全区別す
るもの)を用いて4×4スイツチマトリクスとしたもの
で、回路構成は図示のように簡単である。この図でa1
〜a4は4本の入線、b1〜b4は4本の出線、・点は
ワイヤードオアであり、基本格子は入線の一方を出線の
一方へ、同時に入線の他方を出線の他方へ接続できるか
ら、a!〜a4の任意のものけb1〜b4の任意のもの
へ同時に(勿論二重選択は除いて)接続することができ
る。In a 4F telephone exchange, any one of a large number of incoming lines is connected to any one of a large number of outgoing lines, and while the outgoing line is connected, other people out
Similarly, it is necessary that the blinds can be connected selectively. Such an exchange function can be easily realized using a mechanical type, such as a crossbar switch, or a digital type, such as a highway switch that uses memory. For example, crossbar
In mechanical or electronic switching systems that use switches, it is easy to construct a large-scale switch matrix from a small-scale switch matrix called a basic grid. Figure 1 shows a 4x4 switch matrix using a 2x2 basic lattice 10 (subscripts a, b, etc. are used to distinguish between each other), and the circuit configuration is as shown in the figure. It's as simple as that. In this diagram a1
~a4 is 4 incoming lines, b1 to b4 are 4 outgoing lines, ・The points are wired ORs, and the basic grid connects one of the incoming lines to one of the outgoing lines, and at the same time connects the other incoming line to the other outgoing line. Because I can, a! It is possible to connect any one of ~a4 to any one of b1 to b4 at the same time (excluding double selection, of course).
光通信においても当然交換機能は必要であシ、この場合
も多数の入側光ファイバの任意のもの全多数の出側光フ
ァイバの任意のものへ接続し、そして小規模基本格子金
柑いて容易に大規模スイッチマトリクスを構成できるこ
とが望腫れる。しかし、光基本格子け1×1またけ2×
2などの小規模のものしか作られておらず(クロスバ−
の場合は8×8など)、シかも従来方式では分岐、結合
け1.ないので大規模化は容易でない。Of course, a switching function is necessary in optical communication, and in this case, any one of the many incoming optical fibers can be connected to any one of the many outgoing optical fibers, and it is easy to use a small-scale basic lattice. It is hoped that it will be possible to construct a large-scale switch matrix. However, the basic optical grid is 1×1 and 2×
Only small-scale models such as 2 were made (crossbar
(e.g. 8×8), the conventional method requires branching, joining, etc. Therefore, it is not easy to scale up.
第2図でこの点全説明すると、20ば2×2の光M本格
子であり、(a)はこれを単純に第1図のように4個用
いた場合を示す。分岐、結合けしないから図示のような
結線にしかならず、これでは入線al〜a4の1つ全出
線す、〜b4の1つへ接続することはできるが、ある人
、出線全接続しているとき、他の人、出線′fr:接続
する操作が非常な制約金堂ける。例えばalとblが接
続されているとalとblの接続は不可であり、alが
b3に接続されているならalとb4の接続はできない
。これは前者の例で(はal 。To fully explain this point with reference to FIG. 2, it is a 20×2 x 2 light M-line grating, and (a) shows the case where four of these are simply used as in FIG. 1. Since there is no branching or joining, the only way to connect is as shown in the diagram.With this, it is possible to connect all of the incoming lines al to a4 to one of the outgoing lines and to one of the outgoing lines to b4, but some people have connected all the outgoing lines. When there are other people, the connection operation is extremely restricted. For example, if al and bl are connected, connection of al and bl is impossible, and if al is connected to b3, connection of al and b4 is impossible. This is an example of the former (al.
b、が)しファイバーt+ ’f<使用中であるからa
2’tj’、 t+ f1史用して20bと従ってbl
と接pIcすることができず、後背の例ではal r
a3による光ファイバt2の[史用で、a2+4++b
4の経路が小成〜″rとなることに依る。第2図(b)
に示すように基本格子を2個追加して20a〜2Ofの
6個とすると、−1−記の点はf改善される。即ちal
r b3の回路が20a、2Of、2[]d(または
20a、20e、20d)の経路で成立していてもal
r b4の回路は20a、20e、20d (または
20a、2Of、20d)の経路で成立できる。しかし
al + 20 a + 20 e + 20 d r
b3によりIkl r b3の回路が、まfC&4.
20 c 、 2 Of 、 2 D b 、 blに
よI) a4.blの回路ができているときal r
blの回路(rt光ファイバt3またはt4が使用済み
なので成立できないという問題がある。これは第2図(
c)のように光基本格子全7個使用すると解決できる。b, is) and fiber t+ 'f< is in use, so a
2'tj', 20b and therefore bl using t+f1 history
It is not possible to connect with pIc, and in the rear example, al r
of optical fiber t2 by a3 [for historical purposes, a2+4++b
This depends on the fact that the path of 4 becomes Kosei~''r.Figure 2(b)
If two basic lattices are added to make six basic lattices 20a to 2Of as shown in the figure, the point indicated by -1- is improved by f. That is, al
r Even if the circuit of b3 is established with the paths 20a, 2Of, 2[]d (or 20a, 20e, 20d), al
The circuit of r b4 can be established with paths 20a, 20e, 20d (or 20a, 2Of, 20d). But al + 20 a + 20 e + 20 dr
By b3, the circuit of Ikl r b3 becomes fC&4.
20 c, 2 Of, 2 D b, bl I) a4. When the circuit of bl is created, al r
bl circuit (there is a problem that it cannot be established because the rt optical fiber t3 or t4 is already used. This is shown in Figure 2 (
This problem can be solved by using all seven basic optical lattices as shown in c).
即ち点線りの経路があるのでa2→b1が成立する。光
基本格子をこのように7個用いると第1図の電気的スイ
ッチマトリクスと同様な交換動作を行なうことができる
が、基本格子数が多く、大型、高コストになるのは避け
られない。That is, since there is a dotted route, a2→b1 holds true. Using seven optical elementary gratings in this way allows for the same switching operation as the electrical switch matrix shown in FIG. 1, but it is inevitable that the number of elementary gratings will be large, resulting in large size and high cost.
本発明はか\る点全改善し、簡単な構成で大規模スイッ
チマトリクスを構成可能にしようとするもので、特徴と
する所は初数個の光基本格子全行および列方向にマトリ
クス状に配設し、それぞれ行方向に延びる複数の入41
1tl光ファイバ金光分配器により列数ンrけ分岐して
各列方向に並ぶ各光基本l格子の対応する入線へ接続し
、各列方向に並ぶ各光基本格子の出線はそれぞれ列方向
に延びる複数の共通出側光ファイバの対応するものへ光
結合器により接続してなることにある。第3図〜第5図
にその実施例金星す。The present invention attempts to completely improve these points and to enable the construction of a large-scale switch matrix with a simple configuration. A plurality of inputs 41 are arranged and each extends in the row direction.
The 1TL optical fiber is branched into r rows by a gold optical splitter and connected to the corresponding input line of each basic optical grating arranged in the direction of each column, and the output line of each basic optical grating arranged in the direction of each column is connected to the corresponding input line in the direction of each column. The optical fibers are connected to corresponding ones of a plurality of extending common output optical fibers by optical couplers. Examples of Venus are shown in FIGS. 3 to 5.
第6図は2×2光基本格子ケ4個用いて4×4スイツチ
マトリクスを構成し7た例全示す。a1〜a。FIG. 6 shows all seven examples in which a 4×4 switch matrix is constructed using four 2×2 optical basic lattices. a1~a.
は入111す光ファイバ、bI−b4は出側光ファイバ
、20a〜20dld光基本格子、tけスイッチマ)
IJクス内光ファイバ、22a〜22dけ光分配器、2
4a〜24dは光結合器、26は光増幅器である。Input 111 optical fiber, bI-b4 output optical fiber, 20a to 20dld optical basic grating, t switcher)
Optical fiber in IJ box, optical splitter for 22a to 22d, 2
4a to 24d are optical couplers, and 26 is an optical amplifier.
光基本格子は機械式、電子式などのいずれのものでもよ
く、機械式の場合はマトリクスの各交点に配設された回
転反射鏡全駆動して光伝送路の切換ケ行なう。光分配器
22としては例えば第4図(a)の形式のもの全使用す
る。3oけ光ファイバと同質の光伝送媒体、32はハー
フミラ−である。点線は光ファイバが接続される状態を
示す。今、矢印F+力方向ら光信号が入力したとすると
、ハーフミラ−32によシ半分は透過し、半分は反射し
、矢印1’2+F3で示すように出てゆく。この分岐で
光信号エネルギは半減するから増幅器26で増幅する。The basic optical grating may be of either a mechanical type or an electronic type; in the case of a mechanical type, the optical transmission paths are switched by fully driving the rotary reflecting mirrors disposed at each intersection of the matrix. As the optical distributor 22, for example, one of the type shown in FIG. 4(a) is used. 3 o are optical transmission media of the same quality as optical fibers, and 32 is a half mirror. The dotted line indicates the state in which the optical fiber is connected. Now, if an optical signal is input from the direction of the arrow F+ force, half of it is transmitted through the half mirror 32, the other half is reflected, and the signal goes out as shown by the arrow 1'2+F3. Since the optical signal energy is halved by this branching, it is amplified by the amplifier 26.
第4図(b)は光結合器24の一例を示す。これは2叉
状をなす光伝送媒体で、矢印F!力方向ら入力した光信
号もまた矢印F2方向から入力した光信号も共に矢印F
3方向へ伝送される。FIG. 4(b) shows an example of the optical coupler 24. This is a bifurcated optical transmission medium, with arrow F! Both the optical signal input from the force direction and the optical signal input from the arrow F2 direction are
It is transmitted in three directions.
光増幅器26としては(a)半導体レーザ増幅器、(b
)非線形光学結晶全利用した光増幅器、(c)光ICE
よる増幅モジー−ルなどがある。(、)は閾値附近にバ
イアスされた半導体レーザを増幅器とするものであり、
(b)にはパラメ) IJツク光増幅器や光トランジス
タなどがある。また(c)けGaAsなどの基板正洗検
波器、レーザ、光導波路、トランジスタ増幅器などを集
積化したものである。The optical amplifier 26 includes (a) a semiconductor laser amplifier, (b)
) Optical amplifier that fully utilizes nonlinear optical crystals, (c) Optical ICE
There are various amplification modules. (,) uses a semiconductor laser biased near the threshold as an amplifier,
Parameters in (b) include IJT optical amplifiers and optical transistors. In addition, (c) a substrate such as GaAs is integrated with a detector, a laser, an optical waveguide, a transistor amplifier, etc.
この第6図は結線としては第1図と同じであるから、第
1図と同等の交換機能を発揮することができる。そして
使用光基本格子は4個でよく、第2図(C)のような7
個を必要としない。この有利性は更に大規模化すると益
々顕著になる。嬉5図け2×2光基本格子を用いてろ×
6スイツチマ) IJクスを・構成1〜ン’c例で、准
本格子9個で可能である。Since the wiring connections in FIG. 6 are the same as in FIG. 1, the same exchange function as in FIG. 1 can be achieved. The number of basic optical lattices used can be 4, and 7 as shown in Figure 2 (C).
does not require pieces. This advantage becomes even more noticeable as the scale increases. Please use the 2x2 basic optical lattice for the 5th drawing.
6) In the configurations 1 to 1, it is possible to use 9 quasi-main grids.
8×8スイッチマトリクスは第3 +v+のスイッチマ
トリクスを大基本格子としてそjL?4個、第3図のよ
)に配置、結線して可能である。以下こ扛に僧する。The 8×8 switch matrix is constructed using the third +v+ switch matrix as a large basic lattice. It is possible to arrange and connect four pieces (as shown in Figure 3). The following will be explained to you as a monk.
以上説明したように本発明によれば小規模光基本格子金
柑いて容易に大規模スイッチマトリクスを構成でき、光
通信における交換機能」暑強に寄与する所が大である。As explained above, according to the present invention, a large-scale switch matrix can be easily constructed using a small-scale optical basic lattice lattice, and this greatly contributes to improving the switching function in optical communications.
第1図け′電気スイッチ型基本格子を用いてスイッチマ
トリクスを構成する要領ケ示すブロック図、第2図は光
基本格子を用いてスイッチマトリクスを構成する場合の
説明図、第6図は本発明の一実施++Uを示すブロック
図、第4図はその一部の具体例の説明図、第5図は本発
明の他の実強例を示すブロック図である。
図tl′liで20は基本格子、al〜a6は入側光フ
ァイバ、b1〜b6け出(++:1光ファイバ、22は
光分岐器、24は光結合器で4)る。
出願人 富士通株式会社
代理人非理士 背 柳 稔−よ −ン
4)J)
υ) 対 )Figure 1 is a block diagram illustrating how to configure a switch matrix using an electrical switch type basic lattice, Figure 2 is an explanatory diagram of a switch matrix constructed using an optical basic lattice, and Figure 6 is a block diagram showing the method of configuring a switch matrix using an electrical switch type basic lattice. FIG. 4 is an explanatory diagram of a specific example of a part thereof, and FIG. 5 is a block diagram showing another practical example of the present invention. In FIG. tl'li, 20 is a basic grating, al to a6 are input optical fibers, and b1 to b6 are output (++: 1 optical fiber, 22 is an optical splitter, and 24 is an optical coupler (4)). Applicant Fujitsu Ltd. Representative Minoru Seyanagi, non-physician
4) J) υ) vs.)
Claims (1)
配設し、それぞれ行方向に延びる複数の入側光ファイバ
を光分配器により列数だけ分岐して各列方向に並ぶ各光
基本格子の対応する入線へ接続し、各列方向に並ぶ各光
基本格子の出線はそれぞれ列方向に延びる複数の共通出
側光7アイノ(の対応するものへ光結合器により接続し
てなることを特徴とする光スイツチ装置。A plurality of basic optical gratings are arranged in a matrix in the row and column directions, and a plurality of input optical fibers extending in the row direction are branched by the number of columns by an optical splitter, and each basic optical grating is arranged in the column direction. The outgoing lines of the basic optical grids arranged in each column direction are connected to the corresponding incoming lines of the plurality of common outgoing light beams extending in the column direction (by optical couplers). Characteristic optical switch device.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16833981A JPS5868703A (en) | 1981-10-21 | 1981-10-21 | Optical switch |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16833981A JPS5868703A (en) | 1981-10-21 | 1981-10-21 | Optical switch |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5868703A true JPS5868703A (en) | 1983-04-23 |
Family
ID=15866219
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP16833981A Pending JPS5868703A (en) | 1981-10-21 | 1981-10-21 | Optical switch |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5868703A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2580881A1 (en) * | 1985-04-22 | 1986-10-24 | Cordons Equipements | Intercommunication and data transmission network structured in a distributed star. |
JPS6234497A (en) * | 1985-08-07 | 1987-02-14 | Nec Corp | Optical switch network |
JP2009147880A (en) * | 2007-12-18 | 2009-07-02 | Nippon Telegr & Teleph Corp <Ntt> | 4x4 SWITCH |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5339010A (en) * | 1976-09-22 | 1978-04-10 | Fujitsu Ltd | Switch extending connector system |
JPS53109651A (en) * | 1977-03-08 | 1978-09-25 | Nippon Telegr & Teleph Corp <Ntt> | Optical switch and optical switch matrix |
JPS5488709A (en) * | 1977-12-26 | 1979-07-14 | Nippon Telegr & Teleph Corp <Ntt> | Light exchanging system |
-
1981
- 1981-10-21 JP JP16833981A patent/JPS5868703A/en active Pending
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5339010A (en) * | 1976-09-22 | 1978-04-10 | Fujitsu Ltd | Switch extending connector system |
JPS53109651A (en) * | 1977-03-08 | 1978-09-25 | Nippon Telegr & Teleph Corp <Ntt> | Optical switch and optical switch matrix |
JPS5488709A (en) * | 1977-12-26 | 1979-07-14 | Nippon Telegr & Teleph Corp <Ntt> | Light exchanging system |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2580881A1 (en) * | 1985-04-22 | 1986-10-24 | Cordons Equipements | Intercommunication and data transmission network structured in a distributed star. |
JPS6234497A (en) * | 1985-08-07 | 1987-02-14 | Nec Corp | Optical switch network |
JP2009147880A (en) * | 2007-12-18 | 2009-07-02 | Nippon Telegr & Teleph Corp <Ntt> | 4x4 SWITCH |
JP4586064B2 (en) * | 2007-12-18 | 2010-11-24 | 日本電信電話株式会社 | 4x4 switch |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US5953143A (en) | Multidimensional switching networks | |
US6768573B1 (en) | Polarization control optical space switch | |
JP2626525B2 (en) | Optical interconnection network | |
JPH0349445A (en) | Network communication system with n inlets and m outlets | |
US4917456A (en) | Optical crossover network | |
US6473211B2 (en) | Optical crossbar switching and/or routing system | |
JPS5868703A (en) | Optical switch | |
WO2021018286A1 (en) | Optical cross-connect apparatus | |
JPH0778590B2 (en) | Optical switch array | |
KR20010090766A (en) | Integrated optical switch array | |
AU3898099A (en) | Integrated optical switch array | |
JP2774630B2 (en) | Optical signal path switching device | |
JPS6370693A (en) | Optical matrix switch device | |
KR20010043658A (en) | Integrated Optical Switch Array | |
JP3197611B2 (en) | Multi-terminal optical switch | |
JPS58122513A (en) | Optical star coupler | |
JP3023221B2 (en) | Multi-terminal optical switch | |
JPH1066112A (en) | Optical matrix switch | |
JPH03101716A (en) | Optical switch, optical switch array, and multi-port optical switch | |
JPH0430130A (en) | Optical switch | |
JPH0515119B2 (en) | ||
RU2042167C1 (en) | Optical channel switch for commutators of two-dimensional images | |
JP2613405B2 (en) | Two-dimensional optical time switch device | |
JPS6365428A (en) | Optical matrix switch | |
JPH0792576B2 (en) | 3D optical matrix switch |